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Número de publicaciónUS4525843 A
Tipo de publicaciónConcesión
Número de solicitudUS 06/373,188
Fecha de publicación25 Jun 1985
Fecha de presentación29 Abr 1982
Fecha de prioridad29 Abr 1982
TarifaCaducada
Número de publicación06373188, 373188, US 4525843 A, US 4525843A, US-A-4525843, US4525843 A, US4525843A
InventoresJean-Claude Diels
Cesionario originalThe United States Of America As Represented By The Secretary Of The Navy
Exportar citaBiBTeX, EndNote, RefMan
Enlaces externos: USPTO, Cesión de USPTO, Espacenet
Ring laser with wavefront conjugating beams
US 4525843 A
Resumen
An improvement for a ring laser gyro employs insertion of a wavefront conjugating coupling element inside a laser cavity to reduce the lock-in threshold and to reduce the imbalance between the amplitudes of the opposite direction traveling waves (ODTW) in homogeneously broadened rotating ring lasers.
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Reclamaciones(5)
I claim:
1. An improvement for a ring laser gyro which reduces the lock-in frequency comprising: a gain medium coupled between two optical cavity means, one cavity means forming a closed optical ring with counter wave propagations inv said ring, an the other optical cavity means being off axis to said leg containing said gain medium and forming a short linear resonant cavity, whereby wave mixing of radiation in said ring and radiations in said resonant cavity produces wave front conjugation to reduce lock in frequency of said ring laser gyro.
2. An improvement for a ring laser gyro which reduces the lock-in frequency comprising:
a first optical cavity means forming a closed optical ring containing a gain medium in one leg of said ring and a non-linear medium in a different leg of said ring and having counter wave propagation,
a second optical cavity means also containing said non-linear medium, said second optical cavity means delimiting said non-linear medium by a totally reflective mirror at one end and an external laser source at the other end, said second optical cavity means being off axis with respect to said first optical cavity at said different leg of said ring,
whereby wave mixing of radiation from said gain medium in said ring and radiation from said non-linear medium in the different leg of said ring produces wave front conjugation to reduce lock-in frequency of said ring laser gyro.
3. The improvement of claim 2 wherein said non-linear medium is a metal vapor.
4. The improvement of claim 3 wherein said metal vapor is mercury vapor.
5. An improvement for a ring laser gyro which reduces the lock-in frequency comprising:
a first optical cavity means forming a closed optical ring containing a gain medium in one leg of said ring and having counter wave propagations,
a second optical cavity means contained within said ring at an apex of said ring and including a waveguide laser having two totally reflective means being disposed on end of and external to said waveguide laser,
said waveguide laser being pumped by an external radiation source,
said waveguide laser also containing a rotating mirror which forms an integral part of the chamber of said waveguide,
whereby wave mixing of radiation from said gain medium in said ring and radiation from said second optical cavity means produces wave front conjugation to reduce lock-in frequency of said laser gyro.
Descripción
BACKGROUND OF THE INVENTION

If a ring laser is rotated, the cavity round trip time becomes different for the two oppositely traveling waves (ODTW). This implies the two oppositely traveling waves have to assume different frequencies. If portions of each of the ODTW are allowed to exit the cavity and are mixed, a beat frequency can be detected that is proportional to the applied rotation rate. This is the ideal laser gyro. In practice, however, there is a coupling of the ORTW due to backscattering of one of the ODTW into the other. At low rotation rates, this coupling causes the ODTW to assume the same frequency and the beat frequency disappears. This frequency synchronization of the ODTW is termed lock-in.

A good ring laser for gyro application should not only have a minimal coupling between counterpropagating waves but also have a stable "standing wave" mode of operation when at rest. Homogeneously broadened gain media such as in solid state and dye lasers have therefore been ruled out for gyro operation.

D. Kuhlke and R. Horak, Opt. Quant. Elect. II, 485 (1979) showed for instance that, in the case of cw dye lasers with weak backscattering coupling, there is generally a strong imbalance between the counterpropagating amplitudes. The laser operation even alternates between the two modes when the backscattering coupling exceeds a certain threshold.

SUMMARY OF THE INVENTION

The present invention is directed to an improved ring laser gyro wherein it is possible to use homogeneously broadened lasers such as a solid state or dye laser and provide a substantial reduction in lock-in frequency. This is done by the incorporation of a wavefront conjugating coupling element between the counter wave propagations of a ring laser. Accordingly, an object of the invention is to provide a means of reducing the lock-in threshold of a ring laser gyro.

Another object of the invention is to provide a means of reducing the lock-in threshold of a ring laser gyro by introducing wavefront conjugating therein.

Other objects, advantages and novel features of the invention will become apparent from the following detailed description of the invention when considered in conjunction with the accompanying drawings wherein:

FIG. 1 is a schematic diagram of a ring laser gyro using two coupled cavities to create the wavefront conjugation.

FIG. 2 is a schematic diagram of a ring laser gyro using an external laser, and four wave mixing in a resonant medium to create the wavefront conjugation.

FIG. 3 is a schematic diagram of a ring laser gyro using an external laser, and four wave mixing in a turning mirror to create the wavefront conjugation.

FIG. 4 is an integrated optics modification of the embodiment of FIG. 3.

Referring now to the drawings wherein there is shown in FIG. 1 a typical ring laser, in simplified fashion, as mirrors 10, 12, and 14 and laser gain medium 16. As shown, gain medium 16 has two coupled cavities: one short linear cavity bounding the gain medium, and the ring cavity. Wavefront conjugation arises from the mixing of the two pump beams Ip1 and Ip2 (forming standing waves) with the counterpropagating waves of the ring cavity in the gain medium.

In FIG. 2 an external laser source 20 is provided and four wave mixing in the resonant medium 22 provides the wavefront conjugation. Resonant medium 22 may be a metal vapor such as mercury or in a crystal such as LiTaO3 and CdTe.

In FIG. 3 an external laser is utilized with the four wave mixing being done with a turning mirror 30. The embodiment of FIG. 4 shows how the ring gyro error is detected in an integrated optics system.

In all of the above described FIGS. the embodiments all rely on the incorporation of a wavefront conjugating coupling element between the counterpropagating waves. A discussion of the theory as to how and why the insertion of a conjugating coupling element between the counterpropagating waves will reduce lock-in frequency is given in an article entitled "Influence of Wavefront Conjugated Coupling on the Operation of a Laser Gyro", by Jean-Claude Diels and Ian C. McMichael published in Optics Letters, Vol. 6, No. 5, May 1981, pp 219.

Obviously many modifications and variations of the present invention are possible in the light of the above teachings. It is therefore to be understood that within the scope of the appended claims the invention may be practiced otherwise than as specifically described.

Citas de patentes
Patente citada Fecha de presentación Fecha de publicación Solicitante Título
US4233571 *27 Sep 197811 Nov 1980Hughes Aircraft CompanyLaser having a nonlinear phase conjugating reflector
US4247831 *29 Nov 197827 Ene 1981The Secretary Of State For Defence In Her Britannic Majesty's Government Of The United Kingdom Of Great Britain And Northern IrelandRing lasers
US4429393 *12 Jun 198131 Ene 1984Hughes Aircraft CompanyDouble phase-conjugate ring resonator
Otras citas
Referencia
1Diels et al.; "Influence of Wave-Front-Conjugated Coupling on the Operation of a Laser Gyro"; Opt. Lett., vol. 6, No. 5, May 1981.
2 *Diels et al.; Influence of Wave Front Conjugated Coupling on the Operation of a Laser Gyro ; Opt. Lett., vol. 6, No. 5, May 1981.
3Kaptam et al., "Enhancement of the Sagnac Effect due to Nonlinearly Inducedonreciprocity"; Opt. Lett., vol. 6, No. 12, Dec. 1981.
4 *Kaptam et al., Enhancement of the Sagnac Effect due to Nonlinearly Induced Nonreciprocity ; Opt. Lett., vol. 6, No. 12, Dec. 1981.
Citada por
Patente citante Fecha de presentación Fecha de publicación Solicitante Título
US4659223 *1 Nov 198421 Abr 1987Thomson-CsfPhotorefractive crystal interferometric device for measuring an angular rotational speed
US4739507 *15 Ago 198619 Abr 1988Board Of Trustees, Stanford UniversityDiode end pumped laser and harmonic generator using same
US5004341 *26 Sep 19882 Abr 1991Quantel, S.A.Active optical gyrometer employing a phase conjugation
US5052815 *13 Abr 19901 Oct 1991Coherent, Inc.Single frequency ring laser with two reflecting surfaces
US5121402 *28 Sep 19909 Jun 1992The United State Of America As Represented By The Secretary Of The NavyMultiple element ring laser
US5363192 *28 Jun 19918 Nov 1994Honeywell Inc.Mode-locked active gyro solid state lasers
US5367528 *8 May 199222 Nov 1994Honeywell Inc.Motion induced elimination of dead band in a short pulse laser gyro
US5469460 *9 Sep 199421 Nov 1995U.S. Philips CorporationRing laser
US5563968 *2 Ago 19948 Oct 1996U.S. Philips CorporationMultimode imaging component and ring laser provided with a multimode imaging component
US5640405 *1 Feb 199617 Jun 1997Lighthouse Electronics CorporationMulti quasi phase matched interactions in a non-linear crystal
US5768302 *20 May 199716 Jun 1998Lightwave Electronics CorporationMulti quasi phase matched interactions in a non-linear crystal and method using same
US665068227 Abr 200018 Nov 2003University Of New MexicoBi-directional short pulse ring laser
US7589841 *17 Ago 200715 Sep 2009ThalesSolid-state laser gyro with a mechanically activated gain medium
US857640326 Oct 20095 Nov 2013ThalesLaser gyro having a solid-state amplifying medium and an optical ring cavity
WO1990004867A1 *18 Oct 19893 May 1990Amoco CorpOptical feedback control in the frequency conversion of laser diode radiation
WO1995007562A1 *7 Sep 199416 Mar 1995Philips Electronics NvRing laser
WO2010049372A1 *26 Oct 20096 May 2010ThalesLaser gyro having a solid-state amplifying medium and an optical ring cavity
Clasificaciones
Clasificación de EE.UU.372/94, 372/21, 372/97, 356/472, 356/461, 356/459, 372/64
Clasificación internacionalG01C19/66, H01S3/083
Clasificación cooperativaG01C19/66, H01S3/083
Clasificación europeaG01C19/66, H01S3/083
Eventos legales
FechaCódigoEventoDescripción
14 Sep 1993FPExpired due to failure to pay maintenance fee
Effective date: 19930627
27 Jun 1993LAPSLapse for failure to pay maintenance fees
26 Ene 1993REMIMaintenance fee reminder mailed
11 Jul 1988FPAYFee payment
Year of fee payment: 4
9 Oct 1984ASAssignment
Owner name: UNITED STATES OF AMERICA AS REPRESENTED BY THE SEC
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST. SUBJECT TO LICENSE RECITED.;ASSIGNOR:DIELS, JEAN-CLAUDE;REEL/FRAME:004308/0476
Effective date: 19840830